Baoxing Duan;Jiasen Wang;Chunping Tang;Yintang Yang
{"title":"带有电子控制栅极的新型低导通电压反向导电 LIGBT","authors":"Baoxing Duan;Jiasen Wang;Chunping Tang;Yintang Yang","doi":"10.1109/LED.2024.3435037","DOIUrl":null,"url":null,"abstract":"A novel Reverse-Conducting Lateral Insulated Gate Bipolar Transistor (RC-LIGBT) is proposed and investigated in this letter for the first time, which features the Electron-controlled Gate (EG) and Separated Short-Anode (SSA), named as EGSSA LIGBT. The EG structure is made up of two p-n junctions and is connected to the gate and anode of the device. In the on-state, EG is clamped at a high gate potential. Thus, a high-density electron channel to the anode is formed on the surface of the drift region, which greatly reduces the on-state voltage drop (\n<inline-formula> <tex-math>${V} _{\\text {on}}\\text {)}$ </tex-math></inline-formula>\n of EGSSA LIGBT. Meanwhile, based on the EG structure, a low-doping p-drift can be used, which forms an inverse p-n junction with the \n<inline-formula> <tex-math>$\\text {n} ^{+}$ </tex-math></inline-formula>\n anode. Therefore, it requires only a small additional area to eliminate the snapback voltage and achieve the RC characteristic. In addition, the turn-off loss (\n<inline-formula> <tex-math>${E} _{\\text {off}}\\text {)}$ </tex-math></inline-formula>\n of EGSSA LIGBT is optimized by using a short-circuit anode. As simulation results show, EGSSA LIGBT achieves an extremely small V\n<sub>on</sub>\n of 1.03V, which is 42% and 65% lower than that of Conv. LIGBT and SSA LIGBT at the same \n<inline-formula> <tex-math>${E} _{\\text {off}}$ </tex-math></inline-formula>\n. And at the same \n<inline-formula> <tex-math>${V} _{\\text {on}}$ </tex-math></inline-formula>\n, the \n<inline-formula> <tex-math>${E} _{\\text {off}}$ </tex-math></inline-formula>\n of EGSSA LIGBT is 0.10mJ/cm\n<sup>2</sup>\n, 96% lower than that of Conv. LIGBT. What’s more, the proposed device also achieves lower reverse recovery charge (\n<inline-formula> <tex-math>${Q} _{\\text {rr}}\\text {)}$ </tex-math></inline-formula>\n and smaller RC voltage drop (\n<inline-formula> <tex-math>${V} _{\\text {R}}\\text {)}$ </tex-math></inline-formula>\n than SSA LIGBT.","PeriodicalId":13198,"journal":{"name":"IEEE Electron Device Letters","volume":null,"pages":null},"PeriodicalIF":4.1000,"publicationDate":"2024-07-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Novel Low On-State Voltage Reverse-Conducting LIGBT With an Electron-Controlled Gate\",\"authors\":\"Baoxing Duan;Jiasen Wang;Chunping Tang;Yintang Yang\",\"doi\":\"10.1109/LED.2024.3435037\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A novel Reverse-Conducting Lateral Insulated Gate Bipolar Transistor (RC-LIGBT) is proposed and investigated in this letter for the first time, which features the Electron-controlled Gate (EG) and Separated Short-Anode (SSA), named as EGSSA LIGBT. The EG structure is made up of two p-n junctions and is connected to the gate and anode of the device. In the on-state, EG is clamped at a high gate potential. Thus, a high-density electron channel to the anode is formed on the surface of the drift region, which greatly reduces the on-state voltage drop (\\n<inline-formula> <tex-math>${V} _{\\\\text {on}}\\\\text {)}$ </tex-math></inline-formula>\\n of EGSSA LIGBT. Meanwhile, based on the EG structure, a low-doping p-drift can be used, which forms an inverse p-n junction with the \\n<inline-formula> <tex-math>$\\\\text {n} ^{+}$ </tex-math></inline-formula>\\n anode. Therefore, it requires only a small additional area to eliminate the snapback voltage and achieve the RC characteristic. In addition, the turn-off loss (\\n<inline-formula> <tex-math>${E} _{\\\\text {off}}\\\\text {)}$ </tex-math></inline-formula>\\n of EGSSA LIGBT is optimized by using a short-circuit anode. As simulation results show, EGSSA LIGBT achieves an extremely small V\\n<sub>on</sub>\\n of 1.03V, which is 42% and 65% lower than that of Conv. LIGBT and SSA LIGBT at the same \\n<inline-formula> <tex-math>${E} _{\\\\text {off}}$ </tex-math></inline-formula>\\n. And at the same \\n<inline-formula> <tex-math>${V} _{\\\\text {on}}$ </tex-math></inline-formula>\\n, the \\n<inline-formula> <tex-math>${E} _{\\\\text {off}}$ </tex-math></inline-formula>\\n of EGSSA LIGBT is 0.10mJ/cm\\n<sup>2</sup>\\n, 96% lower than that of Conv. LIGBT. What’s more, the proposed device also achieves lower reverse recovery charge (\\n<inline-formula> <tex-math>${Q} _{\\\\text {rr}}\\\\text {)}$ </tex-math></inline-formula>\\n and smaller RC voltage drop (\\n<inline-formula> <tex-math>${V} _{\\\\text {R}}\\\\text {)}$ </tex-math></inline-formula>\\n than SSA LIGBT.\",\"PeriodicalId\":13198,\"journal\":{\"name\":\"IEEE Electron Device Letters\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":4.1000,\"publicationDate\":\"2024-07-29\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"IEEE Electron Device Letters\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://ieeexplore.ieee.org/document/10613827/\",\"RegionNum\":2,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"ENGINEERING, ELECTRICAL & ELECTRONIC\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE Electron Device Letters","FirstCategoryId":"5","ListUrlMain":"https://ieeexplore.ieee.org/document/10613827/","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
Novel Low On-State Voltage Reverse-Conducting LIGBT With an Electron-Controlled Gate
A novel Reverse-Conducting Lateral Insulated Gate Bipolar Transistor (RC-LIGBT) is proposed and investigated in this letter for the first time, which features the Electron-controlled Gate (EG) and Separated Short-Anode (SSA), named as EGSSA LIGBT. The EG structure is made up of two p-n junctions and is connected to the gate and anode of the device. In the on-state, EG is clamped at a high gate potential. Thus, a high-density electron channel to the anode is formed on the surface of the drift region, which greatly reduces the on-state voltage drop (
${V} _{\text {on}}\text {)}$
of EGSSA LIGBT. Meanwhile, based on the EG structure, a low-doping p-drift can be used, which forms an inverse p-n junction with the
$\text {n} ^{+}$
anode. Therefore, it requires only a small additional area to eliminate the snapback voltage and achieve the RC characteristic. In addition, the turn-off loss (
${E} _{\text {off}}\text {)}$
of EGSSA LIGBT is optimized by using a short-circuit anode. As simulation results show, EGSSA LIGBT achieves an extremely small V
on
of 1.03V, which is 42% and 65% lower than that of Conv. LIGBT and SSA LIGBT at the same
${E} _{\text {off}}$
. And at the same
${V} _{\text {on}}$
, the
${E} _{\text {off}}$
of EGSSA LIGBT is 0.10mJ/cm
2
, 96% lower than that of Conv. LIGBT. What’s more, the proposed device also achieves lower reverse recovery charge (
${Q} _{\text {rr}}\text {)}$
and smaller RC voltage drop (
${V} _{\text {R}}\text {)}$
than SSA LIGBT.
期刊介绍:
IEEE Electron Device Letters publishes original and significant contributions relating to the theory, modeling, design, performance and reliability of electron and ion integrated circuit devices and interconnects, involving insulators, metals, organic materials, micro-plasmas, semiconductors, quantum-effect structures, vacuum devices, and emerging materials with applications in bioelectronics, biomedical electronics, computation, communications, displays, microelectromechanics, imaging, micro-actuators, nanoelectronics, optoelectronics, photovoltaics, power ICs and micro-sensors.